A `A_V -= V_o/V_i | 輸出開路`
B `R_i -= V_i/I_i | 輸出開路 `
C `R_o -= V_o / I_o | 輸出短路`
D `A_i -= I_o / I_i | 輸出短路`
`R_o = V_o / I_o | 輸入短路`
A 100
B 150
C 200
D 250
`g_m` = `I_C/V_T`
`r_π` = `V_T/I_B`
`g_m * r_π ` = `(I_C / V_T)*(V_T/I_B)`
= `I_C / I_B` = β = 60m*2.5k = 150
A 1mA
B 1.5mA
C 2mA
D 4mA
`r_π` = `V_T/I_(BQ)`
= `(26m)/(20μ)`
= 1.3kΩ
交流 `i_b` = `v_(be)/r_π`
= `(13m)/(1.3k)`
= `10μ`
`i_c` = `β * i_b ` = `200*10μ`
= 2mA
A 1mA
B 3mA
C 6mA
D 12mA
`I_o` = `V_o / R_o`
`V_o` = `V_i * A_v`
= 5m * 120 = 0.6V
`I_o` = `0.6 / 200` = 3mA
A 交流的電壓增益會受到射極直流電流大小的影響
B 直流電流會從旁路電容通過,可增加直流的電壓增益
C 對直流的工作點而言,旁路電容為負迴授的電路
D 若將旁路電容移除,直流的工作點會明顯改變
A 400kΩ
B 200kΩ
C 100kΩ
D 1kΩ
化成交流等效電路,如下圖
`R_o` = 1k
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